We define a new variable flavour number scheme for use in deep inelastic scattering, motivated by the need to consistently implement high energy resummations alongside a fixed order QCD expansion. We define the DIS( ) scheme at fixed order, and show how to obtain the small x coefficient functions and heavy flavour matrix elements to leading order in the high energy resummation. We then implement these results in a global fit at LO which includes leading resummations with running coupling corrections. Finally, we address the impact of the resummed results on predictions for the longitudinal structure function. We find that they stabilise the behaviour of FL at small x. Overall, we find that resummations significantly improve the fit to scatt...
At NNLO it is particularly important to have a Variable-Flavour Number Scheme (VFNS) to deal with he...
We present the matching relations of the variable flavor number scheme at next-to-leading order, whi...
We have calculated the first and second order corrections to several deep inelastic sum rules which ...
We define a new variable flavor number scheme for use in deep inelastic scattering, motivated by the...
In order to successfully describe DIS data, one must take heavy quark mass effects into account. Thi...
We extend our previous results on small-x resummation in the pure Yang-Mills theory to full QCD with...
We extend our previous results on small-x resummation in the pure Yang--Mills theory to full QCD wit...
In global fits of parton distribution functions (PDFs) a large fraction of data points, mostly from ...
We have recently proposed a form of high-energy factorization in order to find the small-x behaviour...
A comparison is made between two variable flavor number schemes which describe charm quark productio...
Starting from fixed-order perturbation theory (FOPT) we derive expressions for the heavy-flavour com...
We discuss massive quark effects in the endpoint region $x \to 1$ of inclusive deep inelastic scatte...
We discuss massive quark effects in the end-point region x → 1 of inclusive deep inelastic scatterin...
Starting from fixed-order perturbation theory (FOPT) we derive expressions for the heavy-flavour com...
We present the matching relations of the variable flavor number scheme at next-to-leading order, whi...
At NNLO it is particularly important to have a Variable-Flavour Number Scheme (VFNS) to deal with he...
We present the matching relations of the variable flavor number scheme at next-to-leading order, whi...
We have calculated the first and second order corrections to several deep inelastic sum rules which ...
We define a new variable flavor number scheme for use in deep inelastic scattering, motivated by the...
In order to successfully describe DIS data, one must take heavy quark mass effects into account. Thi...
We extend our previous results on small-x resummation in the pure Yang-Mills theory to full QCD with...
We extend our previous results on small-x resummation in the pure Yang--Mills theory to full QCD wit...
In global fits of parton distribution functions (PDFs) a large fraction of data points, mostly from ...
We have recently proposed a form of high-energy factorization in order to find the small-x behaviour...
A comparison is made between two variable flavor number schemes which describe charm quark productio...
Starting from fixed-order perturbation theory (FOPT) we derive expressions for the heavy-flavour com...
We discuss massive quark effects in the endpoint region $x \to 1$ of inclusive deep inelastic scatte...
We discuss massive quark effects in the end-point region x → 1 of inclusive deep inelastic scatterin...
Starting from fixed-order perturbation theory (FOPT) we derive expressions for the heavy-flavour com...
We present the matching relations of the variable flavor number scheme at next-to-leading order, whi...
At NNLO it is particularly important to have a Variable-Flavour Number Scheme (VFNS) to deal with he...
We present the matching relations of the variable flavor number scheme at next-to-leading order, whi...
We have calculated the first and second order corrections to several deep inelastic sum rules which ...